S. Flugge
Nuclear Reactions II: Theory / Kernreaktionen II: Theorie - Handbuch der Physik Encyclopedia of Physics S. Flugge Softcover reprint of the original 1st ed. 1959 edition

Name: Nuclear Reactions II: Theory / Kernreaktionen II: Theorie - Handbuch der Physik Encyclopedia of Physics
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Author: S. Flugge

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Nuclear Reactions II: Theory / Kernreaktionen II: Theorie - Handbuch der Physik Encyclopedia of Physics

S. Flugge

Softcover reprint of the original 1st ed. 1959 edition

449 one finds that for y = Fo (e) C= :n; V3 [Po (2'Yj) 3 -kjF(i) + (2'Yj)! Fd (2'Yj) 3 -ijF (·m, } 1 ( 14.17) C2 = :n; [ - (2'Yj)! Fd (2'Yj) 3 -ijF(i) + Fo (2'Yj) 3 -~;r(i) J, and if y is to be Go(e), C and Chave the same form with Go (2'Yj) replacing Po (2'Yj) 1 2 and G~(2'Yj) replacing Fd(2'Yj). The values of the functions at eo =2'Yj may be ob tained from (14.8). 1 J. K. TYSON has employed the modified Hankel functions of order one third 2 as solutions of (13.4) to obtain expressions for the Coulomb functions for L =0 which converge near e =2'Yj. His results appear as linear combinations of the real and imaginary parts of n ~(x) = (12)!e- ;/6 [A;{- x) - iB;(-x) J, (14.18) and its derivatives multiplying power series in x = (e - 2'Yj)j(2'Yj)1. For values 1 away from the turning point for L =0, TYSON has obtained forms for Po{e) and Go(e) which are similar to (13.1) to (13.3). The JWKB approximation is again the leading term, and some higher order corrections are given. Expressions similar to Eqs. (14.11) and (14.12) have been obtained by T. D. 3 NEWTON employing the integral representation of (4.4). His results give re presentations of FL(e), Gde) in the vicinity of e=2'Yj [whereas (14.11), (14.12) converge near e=eLJ when L

580 pages, biography

Mediji	Grāmatas Paperback Book (Grāmata ar mīksto vāku un līmēto muguru)
Izlaists	2012. gada 14. jūnijs
ISBN13	9783642459252
Izdevēji	Springer-Verlag Berlin and Heidelberg Gm
Lapas	580
Izmēri	170 × 244 × 30 mm · 929 g
Valoda	Angļu